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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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22 <strong>Fluid</strong> <strong>Mechanics</strong>, <strong>Thermodynamics</strong> <strong>of</strong> <strong>Turbomachinery</strong><br />

Douglas, J. F., Gasiorek, J. M. <strong>and</strong> Swaffield, J. A. (1995). <strong>Fluid</strong> <strong>Mechanics</strong>. Longman.<br />

Greitzer, E. M. (1986). An introduction to unsteady flow in turbomachines. In Advanced Topics<br />

in <strong>Turbomachinery</strong>, Principal Lecture Series No. 2. (D. Japikse, ed.) pp. 2.1–2.29, Concepts ETI.<br />

ISO 31/0 (1981). General Principles Concerning Quantities, Units <strong>and</strong> Symbols. International<br />

St<strong>and</strong>ards Organisation, Paris. (Also published as BS 5775: Part 0: 1982, Specifications for<br />

Quantities, Units <strong>and</strong> Symbols, London, 1982).<br />

Pearsall, I. S. (1966). The design <strong>and</strong> performance <strong>of</strong> supercavitating pumps. Proc. <strong>of</strong> Symposium<br />

on Pump Design, Testing <strong>and</strong> Operation, N.E.L., Glasgow.<br />

Pearsall, I. S. (1967). Acoustic detection <strong>of</strong> cavitation. Symposium on Vibrations in Hydraulic<br />

Pumps <strong>and</strong> Turbines. Proc. Instn. Mech. Engrs., London, 181, Pt. 3A.<br />

Pearsall, I. S. <strong>and</strong> McNulty, P. J. (1968). Comparison <strong>of</strong> cavitation noise with erosion. Cavitation<br />

Forum, 6–7, Am. Soc. Mech. Engrs.<br />

Pearsall, I. S. (1972). Cavitation. M & B Monograph ME/10. Mills & Boon.<br />

Quantities, Units <strong>and</strong> Symbols (1975). A report by the Symbols Committee <strong>of</strong> the Royal Society,<br />

London.<br />

Reynolds, O. (1882). On the internal cohesion <strong>of</strong> fluids. Mem. Proc. Manchester Lit. Soc., 3rd<br />

Series, 7, 1–19.<br />

Ryley, D. J. (1980). Hydrostatic stress in water. Int. J. Mech. Eng. Educ., 8 (2).<br />

Shames, I. H. (1992). <strong>Mechanics</strong> <strong>of</strong> <strong>Fluid</strong>s. McGraw-Hill.<br />

Shepherd, D. G. (1956). Principles <strong>of</strong> <strong>Turbomachinery</strong>. Macmillan.<br />

Taylor, E. S. (1974). Dimensional Analysis for Engineers. Clarendon.<br />

The International System <strong>of</strong> Units (1986). HMSO, London.<br />

Wislicenus, G. F. (1947). <strong>Fluid</strong> <strong>Mechanics</strong> <strong>of</strong> <strong>Turbomachinery</strong>. McGraw-Hill.<br />

Young, F. R. (1989). Cavitation. McGraw-Hill.<br />

Problems<br />

1. A fan operating at 1750 rev/min at a volume flow rate <strong>of</strong> 4.25 m 3 /s develops a head <strong>of</strong> 153<br />

mm measured on a water-filled U-tube manometer. It is required to build a larger, geometrically<br />

similar fan which will deliver the same head at the same efficiency as the existing fan, but at a<br />

speed <strong>of</strong> 1440 rev/min. Calculate the volume flow rate <strong>of</strong> the larger fan.<br />

2. An axial flow fan 1.83 m diameter is designed to run at a speed <strong>of</strong> 1400 rev/min with an<br />

average axial air velocity <strong>of</strong> 12.2 m/s. A quarter scale model has been built to obtain a check on<br />

the design <strong>and</strong> the rotational speed <strong>of</strong> the model fan is 4200 rev/min. Determine the axial air<br />

velocity <strong>of</strong> the model so that dynamical similarity with the full-scale fan is preserved. The effects<br />

<strong>of</strong> Reynolds number change may be neglected.<br />

A sufficiently large pressure vessel becomes available in which the complete model can be<br />

placed <strong>and</strong> tested under conditions <strong>of</strong> complete similarity. The viscosity <strong>of</strong> the air is independent<br />

<strong>of</strong> pressure <strong>and</strong> the temperature is maintained constant. At what pressure must the model be tested?<br />

3. A water turbine is to be designed to produce 27 MW when running at 93.7 rev/min under<br />

a head <strong>of</strong> 16.5 m. A model turbine with an output <strong>of</strong> 37.5 kW is to be tested under dynamically<br />

similar conditions with a head <strong>of</strong> 4.9 m. Calculate the model speed <strong>and</strong> scale ratio. Assuming a<br />

model efficiency <strong>of</strong> 88%, estimate the volume flow rate through the model.<br />

It is estimated that the force on the thrust bearing <strong>of</strong> the full-size machine will be 7.0 GN. For<br />

what thrust must the model bearing be designed?<br />

4. Derive the non-dimensional groups that are normally used in the testing <strong>of</strong> gas turbines<br />

<strong>and</strong> compressors.<br />

A compressor has been designed for normal atmospheric conditions (101.3 kPa <strong>and</strong> 15°C). In<br />

order to economise on the power required it is being tested with a throttle in the entry duct to

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